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Freely suspended films of the material DOBAMBC (p-decyloxybenzylidene-p^'-amino 2-methyl butyl cinnamate), which has a layered ferroelectric liquid-crystalline phase (the chiral smectic C phase), are created across a rectangular hole in a glass microscope cover slide. The films are quantized in thickness, being one, two, three, or more monomolecular (smectic) layers thick. In the tilted smectic C phase, the films exhibit a net spontaneous electric polarization parallel to the smectic layers and in the plane of the film. A unique determination of the polarization, the Frank elastic constants, and the associated viscosities is made by comparing intensities of quasielastic Rayleigh-scattered light from orientational fluctuations of the molecular director in the presence and absence of an applied electric field. Measurements are performed on films three smectic layers thick as a function of temperature near the C-A transition. The relevence of our results to the theories of the classical two-dimensional XY transition will be discussed.
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Rosenblatt et al. (1980) studied this question.
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